Dependence on laser intensity and pulse duration in proton acceleration by irradiation of ultrashort laser pulses on a Cu foil target

2005 ◽  
Vol 12 (7) ◽  
pp. 073102 ◽  
Author(s):  
Y. Oishi ◽  
T. Nayuki ◽  
T. Fujii ◽  
Y. Takizawa ◽  
X. Wang ◽  
...  

2004 ◽  
Vol 84 (22) ◽  
pp. 4445-4447 ◽  
Author(s):  
S. M. Wiggins ◽  
J. Solis ◽  
C. N. Afonso


2009 ◽  
Vol 27 (4) ◽  
pp. 611-617 ◽  
Author(s):  
T.P. Yu ◽  
M. Chen ◽  
A. Pukhov

AbstractWe study proton acceleration from a foil target with a transversely varying density using multi-dimensional Particle-in-Cell (PIC) simulations. In order to reduce electron heating and deformation of the target, circularly polarized Gaussian laser pulses at intensities on the order of 1022 Wcm−2 are used. It is shown that when the target density distribution fits that of the laser intensity profile, protons accelerated from the center part of the target have quasi-monoenergetic spectra and are well collimated. In our two-dimensional PIC simulations, the final peak energy can be up to 1.4 GeV with the full-width of half maximum divergence cone of less than 4°. We observe highly efficient energy conversion from the laser to the protons in the simulations.





2020 ◽  
Vol 38 (2) ◽  
pp. 73-78
Author(s):  
Saurabh Kumar ◽  
Devki Nandan Gupta

AbstractThe energy of protons accelerated by ultra-intense lasers in the target normal sheath acceleration (TNSA) mechanism can be greatly enhanced by the laser parameter optimization. We propose to investigate the optimization of laser parameters for proton acceleration using double laser pulses in TNSA mechanism. The sheath field generation at the rear side of the target is significantly affected by the introduction of second laser pulse in TNSA mechanism, and consequently, the energy of the accelerated protons is also modified. The second laser pulse was introduced with different delays to study its impact on proton acceleration. Our study shows that the interplay of laser intensity and pulse duration of both laser pulses affects the proton acceleration. It was found that the proton maximum energy is the function of both laser intensity and pulse duration. A number of simulations have been performed to obtain maximum proton energy data under different combinations of laser intensity and pulse duration for the two laser pulses. The simulation results account for the underline physics for the proton bunch energy and the sheath field as a function of pulse intensity and pulse delay.



2014 ◽  
Vol 90 (2) ◽  
Author(s):  
M. Tayyab ◽  
S. Bagchi ◽  
B. Ramakrishna ◽  
T. Mandal ◽  
A. Upadhyay ◽  
...  


2021 ◽  
Vol 19 (1) ◽  
pp. 015602
Author(s):  
S Shelygina ◽  
V Kompanets ◽  
E Tolordava ◽  
S Gonchukov ◽  
S Chekalin ◽  
...  

Abstract Dynamic optical density spectra were obtained under multipulse excitation of bacterial cultures of S. aureus and P. aeruginosa by 3 μm mid-infrared ultrashort laser pulses, corresponding to the vibrational excitation of the C–H bonds of the bacterial cell. These spectra demonstrated pronounced laser intensity-dependent blue spectral shift, presumably associated with the breaking of hydrogen bonds, which are responsible for the formation of secondary and tertiary protein structures.



2016 ◽  
Vol 25 (03) ◽  
pp. 1650040 ◽  
Author(s):  
V. M. Petrović ◽  
T. B. Miladinović

In this paper, we use semiclassical model to discusse the kinetic electron energy distribution in the single tunnel ionization process of an atom with respect on the pulse duration and the spatial–temporal laser beam distribution. Our theoretical study show that the pulse duration is an important parameter in the ionization process, as well as beam shape.



Author(s):  
Jurgen Boker ◽  
Marco Swantusch ◽  
Toma Toncian ◽  
Mirela Cerchez ◽  
Monika Toncian ◽  
...  


Author(s):  
Isamu Miyamoto ◽  
Kristian Cvecek ◽  
Yasuhiro Okamoto ◽  
Michael Schmidt ◽  
Henry Helvajian




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